In the absence of strain it is known that when the nodes are oriented along the same direction (\(t^1_z = t^{-1}_z\) ), the linear component of the longitudinal magnetoconductivity does not survive as the contributions from both nodes cancel out [1]}, [2]}, [3]}. Hence, as expected, only strong sign-reversal is observed as a function of intervalley scattering strength. Now, in the presence of only strain induced field, such cancellation does not occur and one observes weak sign-reversal as a function of the tilt parameter. Furthermore, in the presence of \(B_5\) -field and absence of external magnetic field, we observe both strong and weak sign-reversal. To illustrate this, in Fig. REF  we plot LMC for a tilted TR broken WSM when the tilts are oriented in the same direction. When both magnetic field and strain induced chiral magnetic field are present, the combination of two can give rise to interesting features. In Fig. REF  we plot the quadratic coefficient \(\sigma _{zz}^{(2)}\)  as a function of both tilt and intervalley scattering strength in the presence of a \(B_5\)  field. We note that the presence of the tilt parameter curves the contour \(\alpha _c\)  separating the two strong sign-reversed regions, i.e., \(\alpha _c = \alpha _c(t_z)\) . The curvature is different when the Weyl cones are oriented opposite to each other or oriented along the same direction.
